Transcript 2/3 - NRG Ljubljana

Spectral functions in NRG
Rok Žitko
Institute Jožef Stefan
Ljubljana, Slovenia
Green's functions - review
+ if A and B are fermionic operators
- if A and B are bosonic operators
Also known as the retarded Green's function.
Following T. Pruschke: Vielteilchentheorie des Festkorpers
NOTE: ħ=1
Laplace transformation:
Inverse Laplace transformation:
Impurity Green's function (for SIAM):
Equation of motion
Example 1:
Example 2:
Example 3: resonant-level model
Here we have set m=0. Actually,
this convention is followed in
the NRG, too.
Hybridization function: fully describes the effect of
the conduction band on the impurity
Spectral decomposition
e=+1 if A and B are fermionic, otherwise e=-1.
spectral representation
e
spectral function
Lehmann representation
Fluctuation-dissipation theorem
Useful for testing the results of spectral-function calculations!
Caveat: G"(w) may have a delta peak at w=0, which NRG will not capture.
Dynamic quantities: Spectral density
Spectral density/function:
Describes single-particle excitations: at which energies it is
possible to add an electron (ω>0) or a hole (ω<0).
Traditional way: at NRG step N we take excitation
energies in the interval [a wN: a L1/2 wN] or [a wN: a
L wN], where a is a number of order 1. This defines
the value of the spectral function in this same
interval.
Patching
1,...,N
E
N+1
E
Patching
1,...,N
E
pL1/2
N+1
E
p
pL
p: patching parameter (in units of energy scale at N+1-th iteration)
Broadening:
traditional log-Gaussian
smooth=old
Broadening:
modified log-Gaussian
smooth=wvd
for x<w0, 1 otherwise.
Broadening:
modified log-Gaussian
smooth=new
Produces smoother spectral functions at finite temperatures (less artifacts at w=T).
Other kernels
smooth=newsc
For problems with a superconducting gap (below W).
smooth=lorentz
If a kernel with constant width is required (rarely!).
Log-Gaussian broadening
1) Features at w=0
2) Features at w≠0
Equations of motion for SIAM:
Self-energy trick
Non-orthodox approach:
analytic continuation usng Padé approximants
We want to reconstruct G(z) on the real axis. We do that by fitting a rational function to
G(z) on the imaginary axis (the Matsubara points). This works better than expected.
(This is an ill-posed numerical problem. Arbitrary-precision numerics is required.)
Ž. Osolin, R. Žitko, arXiv:1302.3334
Kramers-Kronig transformation
Inverse-square-root asymptotic behavior
Inverse square root behavior also found using the
quantum Monte Carlo (QMC) approach:
Silver, Gubernatis, Sivia, Jarrell, Phys. Rev. Lett. 65 496
(1990)
Anderson orthogonality catastrophe physics
Doniach, Šunjić 1970 J. Phys. C: Solid State Phys. 3 285
Arguments:
• Kondo model features characteristic logarithmic behavior, i.e., as a
function of T, all quantities are of the form [ln(T/TK)]-n.
• Better fit to the NRG data than the Doniach-Šunjić form.
(No constant term has to be added, either.)
Osolin, Žitko, 2013
Comparison with experiment?
Excellent agreement
(apart from asymmetry,
presumably due to some
background processes)
NRG calculation
Experiment, Ti (S=1/2) on CuN/Cu(100) surface
A. F. Otte et al., Nature Physics 4, 847 (2008)
Kondo resonance is
not a simple
Lorentzian,
it has
inverse-square-root
tails!
1/w tail
Fano-like interference process between
resonant and background scattering:
RŽ, Phys. Rev. B 84, 195116 (2011)
Density-matrix NRG
• Problem: Higher-energy parts of the spectra
calculated without knowing the true ground
state of the system
• Solution: 1) Compute the density matrix at the
temperature of interest. It contains full
information about the ground state. 2)
Evaluate the spectral function in an additional
NRG run using the reduced density matrix
instead of the simple Boltzmann weights.
W. Hofstetter, PRL 2000
DMNRG for non-Abelian symmetries: Zitko, Bonca, PRB 2006
Spectral function computed as:
W. Hofstetter, PRL 2000
Construction of the complete basis set
Completeness relation:
Complete-Fock-space NRG:
Anders, Schiller, PRL 2005, PRB 2006
Peters, Pruschke, Anders, PRB 2006
Full-density-matrix NRG:
Weichselbam, von Dellt, PRL 2007
Costi, Zlatić, PRB 2010
CFS vs. FDM vs. DMNRG
• CFS and FDM equivalent at T=0
• FDM recommended at T>0
• CFS and FDM are slower than DMNRG
(all states need to be determined, more
complex expressions for spectral functions)
• No patching, thus no arbitrary parameter as in
DMNRG
Error bars in NRG?
Rok Žitko, PRB 84, 085142 (2011)
Average + confidence region!
Effect of the magnetic field:
resonance splitting
Ti atom
S=1/2
A. F. Otte et al., Nature Physics 4, 847 (2008)
Numerical renormalization group (NRG) calculation
Bethe Ansatz calculation using spinon density of states
Exact result for B→0: Δ=(2/3)gmBB
Suggestion that for large B, Δ is larger than gmBB.
gives 2/3 for R=2,
in agreement with
Logan et al. (Factor 2
due to different convention.)
Also find that Δ > 1gmBB, but they note that this
might be non-universal behavior due to charge fluctuations in
the Anderson model (as opposed to the Kondo model).
Interrelated problems: systematic discretization errors
and spectral broadening
a determines how d peaks are smoothed out!
Pessimistic error bars
Rok Žitko, PRB 84, 085142 (2011)
The correct result is obtained in the a→0 limit!
Optimistic error bars
Agreement within error bars!
NRG
B=7 T
Experimental results
for Ti adatoms:
F. Otte et al.,
Nature Physics 4,
847 (2008)
NRG calculation
R. Ž., submitted
Kondo model